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Comparison of microscopic models for disorder in bilayer graphene: Implications for the density of states and the optical conductivity
Mesoscale and Nanoscale Physics · Submitted 26 Sep 2011
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We find that the qualitative behavior of the two scattering potentials are similar, but that the choice of approximation for the self-energy leads to important differences near the band edge in the gapped case.
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We study the effects of disorder on bilayer graphene using four different microscopic models and directly compare their results. We compute the self-energy, density of states, and optical conductivity in the presence of short-ranged scatterers and screened Coulomb impurities, using both the Born approximation and self-consistent Born approximation for the self-energy. We also include a finite interlayer potential asymmetry which generates a gap between the valence and conduction bands. We find that the qualitative behavior of the two scattering potentials are similar, but that the choice of approximation for the self-energy leads to important differences near the band edge in the gapped case. Finally, we describe how these differences manifest in the measurement of the band gap in optical and transport experimental techniques.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study the effects of disorder on bilayer graphene using four different microscopic models and directly compare their results. | contribution 0.99 | 0.95 | 0.04 | asserted 0.89 |
| s1 | We compute the self-energy, density of states, and optical conductivity in the presence of short-ranged scatterers and screened Coulomb impurities, using both the Born approximation and self-consistent Born approximation for the self-energy. | method 0.98 | 0.96 | 0.04 | asserted 0.96 |
| s2 | We also include a finite interlayer potential asymmetry which generates a gap between the valence and conduction bands. | method 0.90 | 0.88 | 0.03 | asserted 0.99 |
| s3 | We find that the qualitative behavior of the two scattering potentials are similar, but that the choice of approximation for the self-energy leads to important differences near the band edge in the gapped case. | result 0.99 | 0.96 | 0.77 | asserted 1.00 |
| s4 | Finally, we describe how these differences manifest in the measurement of the band gap in optical and transport experimental techniques. | interpretation 0.87 | 0.87 | 0.18 | asserted 0.96 |
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Original abstract
We study the effects of disorder on bilayer graphene using four different microscopic models and directly compare their results. We compute the self-energy, density of states, and optical conductivity in the presence of short-ranged scatterers and screened Coulomb impurities, using both the Born approximation and self-consistent Born approximation for the self-energy. We also include a finite interlayer potential asymmetry which generates a gap between the valence and conduction bands. We find that the qualitative behavior of the two scattering potentials are similar, but that the choice of approximation for the self-energy leads to important differences near the band edge in the gapped case. Finally, we describe how these differences manifest in the measurement of the band gap in optical and transport experimental techniques.
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We include the disorder through a constant broadening of the bands parameterized by the energy $Γ$ which appears in the Green's function as [equation] The optical conductivity is calculated from this Green's function from the following expression [ref] : [equation] where $g_s$ and $g_v$ are the spin and valley degeneracies, and [equation] Figure [ref] shows that for $Γ=1$, the peak due to the onset of the intraband conductivity is already significantly blurred.
dmu/dn In suspended bilayer graphene: the interplay of disorder and band gap · Introduction · 0.92
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